Dielectric properties of carbon nanotubes from first principles

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Alignment of graphene nanoribbons by an electric-field (2009, background): “ω = M K = E(2)(α// − α⊥) sin [2(θ0 − θ)] 2K (1) where M is the bending moment induced by the electric polarization [30], 58 K denotes the effective bending stiffness of GNR, L stands for the graphene 59 length, θ is the deflection angle of GNR, E = |E|, and θ0 represent the 60 strength and the direc”
Improving the Toughness and Electrical Conductivity of Epoxy Nanocomposites by using Aligned Carbon Nanofibres (2015, background): “For one-dimensional particles, such as CNFs and CNTs, due to their shape anisotropy the longitudinal polarizability is at least an order of magnitude greater than the transverse polarizability [39,40].”